{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:UD7UDEVFIWEA3HNOPYFH2OBJLA","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"7c59a1445cbb9183ccef39bd625600d0792e48cf20a1f53cc98d5cbd9682c7a0","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-06-30T04:38:19Z","title_canon_sha256":"126ca208611a5802aff48dca9ea32175e87310034796531684ee117ac0393766"},"schema_version":"1.0","source":{"id":"2506.23515","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.23515","created_at":"2026-07-05T11:29:23Z"},{"alias_kind":"arxiv_version","alias_value":"2506.23515v1","created_at":"2026-07-05T11:29:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.23515","created_at":"2026-07-05T11:29:23Z"},{"alias_kind":"pith_short_12","alias_value":"UD7UDEVFIWEA","created_at":"2026-07-05T11:29:23Z"},{"alias_kind":"pith_short_16","alias_value":"UD7UDEVFIWEA3HNO","created_at":"2026-07-05T11:29:23Z"},{"alias_kind":"pith_short_8","alias_value":"UD7UDEVF","created_at":"2026-07-05T11:29:23Z"}],"graph_snapshots":[{"event_id":"sha256:0de6dc691f0bca6b3063812fe0c68abddcafe96ec53eac9c8825973ff2507c37","target":"graph","created_at":"2026-07-05T11:29:23Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2506.23515/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The inverse Faraday effect, the ability of light to act as a source of magnetism, is a cornerstone of modern ultrafast optics. Harnessing this effect at the nanoscale promises to transform data storage and spintronics, yet its predictive understanding remains elusive. This review synthesizes recent progress in engineering the IFE within plasmonic architectures. We bridge the theoretical foundations, from classical drift current models to quantum descriptions, with the latest experimental milestones, including pump probe studies that have verified the effect s subpicosecond nature. Special emph","authors_text":"Chantal Hareau, Maria Sanz, Mathieu Mivelle, Matthew Sheldon, Xingyu Yang","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-06-30T04:38:19Z","title":"Engineering Magnetization with Photons: Nanoscale Advances in the Inverse Faraday Effect for Metallic and Plasmonic Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.23515","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:7224a22af948ad58a99457db8036e2c319cdac4d031cf7f8238654a7e20ce244","target":"record","created_at":"2026-07-05T11:29:23Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"7c59a1445cbb9183ccef39bd625600d0792e48cf20a1f53cc98d5cbd9682c7a0","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-06-30T04:38:19Z","title_canon_sha256":"126ca208611a5802aff48dca9ea32175e87310034796531684ee117ac0393766"},"schema_version":"1.0","source":{"id":"2506.23515","kind":"arxiv","version":1}},"canonical_sha256":"a0ff4192a545880d9dae7e0a7d3829583b9ecdd38f29034a71e23ce0d0ee6353","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a0ff4192a545880d9dae7e0a7d3829583b9ecdd38f29034a71e23ce0d0ee6353","first_computed_at":"2026-07-05T11:29:23.240930Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:29:23.240930Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jSWPXio1wWnp3q0RoTxc046kV//Kvxr6gBGDmbGz9S4eLZak1xKHWBEp6qQdxL81aFdDZMsELlLOMXdi76ZHBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:29:23.241475Z","signed_message":"canonical_sha256_bytes"},"source_id":"2506.23515","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7224a22af948ad58a99457db8036e2c319cdac4d031cf7f8238654a7e20ce244","sha256:0de6dc691f0bca6b3063812fe0c68abddcafe96ec53eac9c8825973ff2507c37"],"state_sha256":"130108d965f76cb2920991dd16a80d19b4a502f89e32a1eec2d2aa83cf66714d"}